Determination of rotational correlation times from deconvoluted fluorescence anisotropy decay curves. Demonstration with 6,7-dimethyl-8-ribityllumazine and lumazine protein from Photobacterium leiognathi as fluorescent indicators

The experimental and analytical protocols required for obtaining rotational correlation times of biological macromolecules from fluorescence anisotropy decay measurements are described. As an example, the lumazine protein from Photobacterium leiognathi was used. This stable protein (Mr 21 200) contains the noncovalently bound, natural fluorescent marker 6,7-dimethyl-8-ribityllumazine, which has in the bound state a long fluorescence lifetime (tau = 14 ns). Shortening of the fluorescence lifetime to 2.6 ns at room temperature was achieved by addition of the collisional fluorescence quencher potassium iodide. The shortening of tau had virtually no effect on the rotational correlation time of the lumazine protein (phi = 9.4 ns, 19 degrees C). The ability to measure biexponential anisotropy decay was tested by the addition of Photobacterium luciferase (Mr 80 000), which forms an equilibrium complex with lumazine protein. Under the experimental conditions used (2 degrees C) the biexponential anisotropy decay can best be described with correlation times of 20 and 60 ns, representing the uncomplexed and luciferase-associated lumazine proteins, respectively. The unbound 6,7-dimethyl-8-ribityllumazine itself (tau = 9 ns) was used as a model compound for determining correlation times in the picosecond time range. In the latter case rigorous deconvolution from the excitation profile was required to recover the correlation time, which was shorter (100-200 ps) than the measured laser excitation pulse width (500 ps).     

Effects of i-propanol on the structural dynamics of Thermomyces lanuginosa lipase revealed by tryptophan fluorescence

Influence of isopropanol (iPrOH) on the structural dynamics of Thermomyces lanuginosa lipase (TLL) was studied by steady-state, time-resolved, and stopped-flow fluorescence spectroscopy, monitoring the intrinsic emission of Trp residues. The fluorescence of the four Trps of the wild-type enzyme report on the global changes of the whole lipase molecule. To monitor the conformational changes in the so-called "lid," an alpha-helical surface loop, the single Trp mutant W89m (W117F, W221H, W260H) was employed. Circular dichroism (CD) spectra revealed that iPrOH does not cause major alterations in the secondary structures of the wild-type TLL and W89m. With increasing [iPrOH], judged by the ratio of emission intensities at 350 nm and 330 nm, the average microenvironment of the Trps in the wild-type TLL became more hydrophobic, whereas Trp89 of W89m moved into a more hydrophilic microenvironment. Time-resolved fluorescence measurements revealed no major changes to be induced by iPrOH neither in the shorter fluorescence lifetime component (tau(1) = 0.5--1.2 ns) for the wild-type TLL nor in the longer fluorescence lifetime component (tau(2) = 4.8--6.0 ns) in the wild-type TLL and the W89m mutant. Instead, for W89m on increasing iPrOH from 25% to 50% the value for tau(1) increased significantly, from 0.43 to 1.5 ns. The shorter correlation time phi(1) of W89m had a minimum of 0.08 ns in 25% iPrOH. Judged from the residual anisotropy r(infinity) the amplitude of the local motion of Trp89 increased upon increasing [iPrOH] 10%. Stopped-flow fluorescence spectroscopy measurements suggested the lid to open within approximately 2 ms upon transfer of W89m into 25% iPrOH. Steady-state anisotropies and longer correlation times revealed increasing concentrations of iPrOH to result also in the formation of dimers as well as possibly also higher oligomers by TLL.     

Influence of immune complexes on macrophage membrane fluidity: a nanosecond fluorescence anisotropy study

Time-resolved fluorescence anisotropy (TRFA) and steady-state anisotropy measurements and fluorescence intensification microscopic observations were made on RAW264 macrophages labeled with 1,6-diphenyl-1,3,5-hexatriene (DPH) or 1-[4-(trimethylammonio)phenyl]-6-phenyl-1,3,5-hexatriene (TMA-DPH). Microscopic analysis revealed that the fluorescent probe DPH was found in association with plasma membranes and small vesicles. Macrophages treated with immune complexes could not be distinguished from untreated cells, indicating that the same membrane compartments were labeled. The probe TMA-DPH was exclusively localized to the plasma membrane. Steady-state anisotropy measurements indicated that in vitro culture conditions did not significantly affect membrane fluidity. TRFA measurements were conducted to determine the physical properties of macrophage membranes during immune recognition and endocytosis. Data were analyzed by iterative deconvolution to yield phi, the rotational correlation time, and r infinity, the limiting anisotropy. These parameters may be interpreted as the "fluidity" and order parameter of the membrane environment, respectively. Typical values for untreated macrophages were phi = 7.8 ns and r infinity = 0.12. Binding and endocytosis of immune complexes prepared in 4-fold antigen excess increase these values to phi = 22.1 ns and r infinity = 0.15. However, receptor-independent phagocytosis of latex beads decreases these values to phi = 2.2 ns and r infinity = 0.10. Addition of catalase before, but not after, immune complex incubation with cells diminishes the effect upon membrane structure, suggesting that H2O2 participates in fluidity changes. Pretreatment of macrophages with the membrane-impermeable sulfhydryl blocker p-(chloromercuri)benzenesulfonic acid also diminished these effects.(ABSTRACT TRUNCATED AT 250 WORDS)     

Time-resolved fluorescence studies of dityrosine in the outer layer of intact yeast ascospores.

The (time-resolved) fluorescence properties of dityrosine in the outermost layer of the spore wall of Saccharomyces cerevisiae were investigated. Steady-state spectra revealed an emission maximum at 404 nm and a corresponding excitation maximum at 326 nm. The relative fluorescence quantum yield decreased with increasing proton concentration. The fluorescence decay of yeast spores was found to be nonexponential and differed pronouncedly from that of unbound dityrosine in water. Analysis of the spore decay recorded at lambda ex = 323 nm and lambda em = 404 nm by an exponential series (ESM) algorithm revealed a bimodal lifetime distribution with maxima centered at tau 1C = 0.5 ns and tau 2C = 2.6 ns. The relative amplitudes of the two distributions are shown to depend on the emission wavelength, indicating contributions from spectrally different dityrosine chromophores. On quenching the spore fluorescence with acrylamide, a downward curvature of the Stern-Volmer plot was obtained. A multitude of chromophores more or less shielded from solvent in the spore wall is proposed to account for the nonlinear quenching of the total spore fluorescence. Analysis of the fluorescence anisotropy decay revealed two rotational correlation times (phi 1 = 0.9 ns and phi 2 = 30.6 ns) or a bimodal distribution of rotational correlation times (centers at 0.7 ns and 40 ns) when the data were analyzed by the maximum entropy method (MEM). We present a model that accounts for the differences between unbound (aqueous) and bound (incorporated in the spore wall) dityrosine fluorescence. The main feature of the photophysical model for yeast spores is the presence of at least two species of dityrosine chromophores differing in their chemical environments. A hypothetical photobiological role of these fluorophores in the spore wall is discussed: the protection of the spore genome from mutagenic UV light.     

Spectral properties and function of two lumazine proteins from Photobacterium

The spectral properties are compared for two 6,7-dimethyl-8-ribityllumazine proteins from marine bioluminescent bacteria, one from a psychrophile, Photobacterium phosphoreum, and the other from a thermophile, Photobacterium leiognathi. The visible spectral properties, which are the ones by which the protein performs its biological function of bioluminescence emission, are almost the same for the two proteins: at 2 degrees C and 50 mM Pi, pH 7, fluorescence quantum yield phi F = 0.59 and 0.54, respectively; fluorescence lifetime tau = 14.4 and 14.8 ns, respectively; fluorescence maxima, both 475 nm; absorption maximum, 417 and 420 nm, respectively; circular dichroism minima at around 420 nm, both -41 X 10(3) deg cm2 dmol-1. The ligand binding sites therefore must provide very similar environments, and arguments are presented that the bound ligand is relatively exposed to solvent. The dissociation equilibrium was studied by steady-state fluorescence polarization. The thermophilic protein binds the ligand with Kd (20 degrees C) = 0.016 microM, 10 times more tightly than the other protein [Kd (20 degrees C) = 0.16 microM]. The origin of the binding difference probably resides in differences in secondary structure. The tryptophan fluorescence spectra of the two proteins are different, but more significant is an observation of the decay of the tryptophan emission anisotropy. For the psychrophilic lumazine protein this anisotropy decays to zero in 1 ns, implying that its single tryptophan residue lies in a very "floppy" region of the protein. For the other protein, the anisotropy exhibits both a fast component and a slow one corresponding to rotation of the protein as a whole.(ABSTRACT TRUNCATED AT 250 WORDS)     

Independent flexible motion of submolecular domains of the Ca2+,Mg2+-ATPase of sarcoplasmic reticulum measured by time-resolved fluorescence depolarization of site-specifically attached probes

The Ca2+-transporting ATPase of rabbit skeletal muscle sarcoplasmic reticulum was site-specifically labeled with either N-(1-anilinonaphth-4-yl)maleimide (ANM) or 5-[[(iodoacetamido)-ethyl]amino]naphthalene-1-sulfonate (IAEDANS), and the segmental motion of submolecular domains of the ATPase molecule was examined by means of time-resolved and steady-state fluorescence anisotropy measurements. The ANM-binding domain showed wobbling with a rotational relaxation time phi = 69 ns in the absence of free Ca2+ without any independent wobbling of the ANM moiety. The IAEDANS-binding domain showed a significantly slower wobbling with phi = 190 ns in the absence of Ca2+. The present results demonstrated for the first time that the ATPase molecule is composed of distinct domains whose mobilities are considerably different from each other. The binding of Ca2+ to the transport site increased the segmental motion of ANM-labeled domain, leading to a phi value of 65 ns. Solubilization of the ANM-labeled SR membranes by deoxycholate led to a further increase in the segmental flexibility (phi = 48 ns in the absence of free Ca2+), indicating that the mobility of the ANM-binding domain was considerably restricted through interaction with the membrane. The mobility of the ANM-binding domain of solubilized ATPase was also increased to some extent upon binding of Ca2+.     

Flexibility of the molecular forms of acetylcholinesterase measured with steady-state and time-correlated fluorescence polarization spectroscopy

Steady-state and time-correlated fluorescence polarizations have been examined for selected complexes and covalent conjugates of the 11S and (17 + 13)S forms of Torpedo acetylcholinesterase. The 11S form exists as a tetramer of apparently identical subunits, whereas the (17 + 13)S forms contain two or three sets of tetramers disulfide-linked to an elongated collagen-like tail unit. Pyrenebutyl methylphosphonofluoridate and (dansylsulfonamido)pentyl methylphosphonofluoridate were conjugated at the active center serine whereas propidium was employed as a fluorescent ligand for the spatially removed peripheral anionic site. Steady-state polarization of the pyrenebutyl conjugates indicates rotational correlation times of approximately 400 ns for the 11S species and greater than 1100 ns for the (17 + 13)S species. Hence, the tail unit severely restricts rotational motion of the catalytic subunits. Time-correlated fluorescence polarization analysis of the 11S species indicates multiple rotational correlation times. Anisotropy decay of the propidium complex (tau = 6 ns) occurs in exponential manner with a rotational correlation time of approximately 150 ns, while covalent adducts at the active center exhibit rotational correlation times greater than or equal to 300 ns. Anisotropy decay of the (dansylsulfonamido)pentyl conjugate (tau = 16 ns) appears exponential with a correlation time of approximately 320 ns, whereas decay of the pyrenebutyl conjugate (tau = 100 ns) is described by two correlation times, phi S = 18 ns and phi L = 320 ns, of small (15%) and large (85%) amplitudes, respectively. Two limiting models have been considered to explain the results.(ABSTRACT TRUNCATED AT 250 WORDS)     

Molecularly imprinted polymer as storage medium for an analyte

A molecularly imprinted polymer (MIP) able to bind theophylline with a considerable degree of selectivity was prepared through a noncovalent route. The polymer after equilibrating with the template molecule (theophylline) and storage for various periods of time, the amount of theophylline desorbed from the polymer was found to be effectively quantitative indicating that MIPs could be used as a storage matrix for analytes. The stored analyte could be desorbed and analysed conveniently.     

Tryptophan dynamics of the FK506 binding protein: time-resolved fluorescence and simulations.

The FK506-binding protein (FKBP12) is important in the immunosuppressant action of FK506 and rapamycin. We have investigated Trp side chain dynamics in FKBP12, with and without a bound immunosuppressant, by measuring the Trp time-resolved fluorescence anisotropy decay r(t). The r(t) for W59 in aqueous uncomplexed FKBP12 at 20 degrees C is well described by a single exponential with a recovered initial anisotropy, r(eff)o, of 0.192 and an overall rotational correlation time for the protein, phi p, of 4.7 ns; r(eff)o = 0.214 and phi p = 4.2 ns for the FKBP12/FK506 complex. Using an expression for the order parameter squared, namely S2 = r(eff)o/rTo, where rTo is the vitrified steady-state excitation anisotropy, we recovered an S2 of 0.75 for W59 fluorescence in uncomplexed FKBP12 and S2 approximately equal to 1 in the FKBP12/FK506 complex. Results obtained for the FKBP12/rapamycin complex are similar to those found for the FKBP12/FK506 complex. Minimum perturbation mapping simulations were performed on the free and complexed forms of FKBP12 and the results were generally in agreement with the experimental data.     

Submicrosecond phospholipid dynamics using a long-lived fluorescence emission anisotropy probe.

The use of the long-lived fluorescence probe coronene (mean value of tau(FL) approximately 200 ns) is described for investigating submicrosecond lipid dynamics in DPPC model bilayer systems occurring below the lipid phase transition. Time-resolved fluorescence emission anisotropy decay profiles, measures as a function of increasing temperature toward the lipid-phase transition temperature (T(C)), for coronene-labeled DPPC small unilamellar vesicles (SUVs), are best described in most cases by three rotational decay components (phi(i = 3)). We have interpreted these data using two dynamic lipid bilayer models. In the first, a compartmental model, the long correlation time (phi(N)) is assigned to immobilized coronene molecules located in "gel-like" or highly ordered lipid phases (S-->1) of the bilayer, whereas a second fast rotational time (phi(F) approximately 2-5 ns) is associated with probes residing in more "fluid-like" regions (with corresponding lower ordering, S-->0). Interests here have focused on the origins of an intermediate correlation time (50-100 ns), the associated amplitude (beta(G)) of which increases with increasing temperature. Such behavior suggests a changing rotational environment surrounding the coronene molecules, arising from fluidization of gel lipid. The observed effective correlation time (phi(EFF)) thus reflects a discrete gel-fluid lipid exchange rate (k(FG)). A refinement of the compartmental model invokes a distribution of gel-fluid exchange rates (d(S,T)) corresponding to a distribution of lipid order parameters and is based on an adapted Landau expression for describing "gated" packing fluctuations. A total of seven parameters (five thermodynamic quantities, defined by the free energy versus temperature expansion; one gating parameter (gamma) defining a cooperative "melting" requirement; one limiting diffusion rate (or frequency factor: d(infinity))) suffice to predict complete anisotropy decay curves measured for coronene at several temperatures below the phospholipid T(C). The thermodynamic quantities are associated with the particular lipid of interest (in this case DPPC) and have been determined previously from ultrasound studies, thus representing fixed constants. Hence resolved variables are r(O), temperature-dependent gate parameters (gamma), and limiting diffusion rates (d(infinity)). This alternative distribution model is attractive because it provides a general probe-independent expression for distributed lipid fluctuation-induced probe rotational rates occurring within bilayer membranes below the phospholipid phase transition on the submicrosecond time scale.     

Ortho-aminobenzoic acid-labeled bradykinins in interaction with lipid vesicles: fluorescence study

The peptide hormone bradykinin (BK) (Arg(1)-Pro(2)-Pro(3)-Gly(4)-Phe(5)-Ser(6)-Pro(7)-Phe(8)-Arg(9)) and its shorter homolog BK(1-5) (Arg(1)-Pro(2)-Pro(3)-Gly(4)-Phe(5)) were labeled with the extrinsic fluorescent probe ortho-aminobenzoic acid (Abz) bound to the N-terminal and amidated in the C-terminal carboxyl group (Abz-BK-NH(2) and Abz-BK(1-5)-NH(2)). The fragment des-Arg(9)-BK was synthesized with the Abz fluorescent probe attached to the 3-amino group of 2,3-amino propionic acid (DAP), which positioned the Abz group at the C-terminal side of BK sequence, constituting the peptide des-Arg(9)-BK-DAP(Abz)-NH(2). The spectral characteristics of the probe were similar in the three peptides, and their fluorescent properties were monitored to study the interaction of the peptides with anionic vesicles of dimyristoylphosphatidylglycerol (DMPG). Time-resolved fluorescence experiments showed that the fluorescence decay of the peptides was best described by double-exponential kinetics, with mean lifetimes values around 8.0 ns in buffer pH 7.4 that increased about 10% in the presence of DMPG vesicles. About a 10-fold increase, compared with the values in aqueous solution, was observed in the steady-state anisotropy in the presence of vesicles. A similar increase was also observed for the rotational correlation times obtained from time-resolved anisotropy decay profiles, and related to the overall tumbling of the peptides. Equilibrium binding constants for the peptide-lipid interaction were examined monitoring anisotropy values in titration experiments and the electrostatic effects were evaluated through Gouy-Chapman potential calculations. Without corrections for electrostatic effects, the labeled fragment Abz-BK(1-5)-NH(2) presented the major affinity for DMPG vesicles. Corrections for the changes in peptide concentration due to electrostatic interactions suggested higher affinity of the BK fragments to the hydrophobic phase of the bilayer.     

Molecular imprinting and solid phase extraction of flavonoid compounds

Molecularly imprinted polymers (MIPs) for quercetin have been successfully prepared by a thermal polymerization method using 4-vinylpyridine (4-VP) and ethylene glycol dimethacrylate (EDMA) as functional monomer and cross-linker, respectively. The obtained molecularly imprinted polymers were evaluated by HPLC using organic eluents, with respect to their selective recognition properties for quercetin and related compounds of the flavonoid class. Two equivalent control polymers, a blank polymer and a polymer imprinted with a structural analogous template, were synthesized, in order to confirm the obtained results. Furthermore, preliminary experiments confirm the applicability of the prepared MIPs for solid phase extraction (SPE), as rapid and facile clean-up of wine samples for HPLC analysis is an envisaged field of application. The successful preparation of molecularly imprinted polymers for flavones provides an innovative opportunity for the development of advanced separation materials, with applications in the field of wine and fermentation analysis.     

Fluorescence properties of methyl 8-(2-anthroyl) octanoate, a solvatochromic lipophilic probe.

Fluorescence excitation and emission spectra, relative fluorescence quantum yield phi r and fluorescence lifetime tau of methyl 8-(2-anthroyl)-octanoate have been studied in a set of organic solvents covering a large scale of polarity and in the presence of water. In this probe, the 2-anthroyl chromophore exhibits quite remarkable and unique fluorescence properties. Thus, when going from n-hexane to methanol, the maximum emission wavelength lambda em max shifts from 404 nm to 492 nm while phi r and tau increase from 1 to 17.7 and from 0.91 ns to 13.5 ns, respectively. These increments are still more accentuated in the presence of water with estimated values of 526 nm for lambda em max, 27 for phi r and 20 ns for tau in this solvent. Because of the presence of a keto group which is a hydrogen bond acceptor and which can conjugate with the aromatic ring so as to provide the chromophore with a high dipole moment, the fluorescence properties of the probe strongly depend on the polarity of the surrounding medium. They can be accounted for in terms of general solvent effects (dipolar solute/solvent interactions) in the presence of aprotic solvents and in terms of specific solvent effects (hydrogen bonding) in protic solvents. Such properties of solvatochromism make the 2-anthroyl chromophore, after 8-(2-anthroyl)octanoic acid has been attached to phospholipids (E. Perochon and J.F. Tocanne (1991) Chem. Phys. Lipids 58, 7-17) a potential tool for studying microenvironmental polarity in biological membranes.     

Modeling HIV-1 integrase complexes based on their hydrodynamic properties

We present a model structure of a candidate tetramer for HIV-1 integrase. The model was built in three steps using data from fluorescence anisotropy, structures of the individual integrase domains, cross-linking data, and other biochemical data. First, the structure of the full-length integrase monomer was modeled using the individual domain structures and the hydrodynamic properties of the full-length protein that were recently measured by fluorescence depolarization. We calculated the rotational correlation times for different arrangements of three integrase domains, revealing that only structures with close proximity among the domains satisfied the experimental data. The orientations of the domains were constrained by iterative tests against the data on cross-linking and footprinting in integrase-DNA complexes. Second, the structure of an integrase dimer was obtained by joining the model monomers in accordance with the available dimeric crystal structures of the catalytic core. The hydrodynamic properties of the dimer were in agreement with the experimental values. Third, the active sites of the two model dimers were placed in agreement with the spacing between the sites of integration on target DNA as well as the integrase-DNA cross-linking data, resulting in twofold symmetry of a tetrameric complex. The model is consistent with the experimental data indicating that the F185K substitution, which is found in the model at a tetramerization interface, selectively disrupts correct complex formation in vitro and HIV replication in vivo. Our model of the integrase tetramer bound to DNA may help to design anti-integrase inhibitors.     

Characterisation of the lowest singlet and triplet excited states of S-flurbiprofen.

The photophysical properties of S-flurbiprofen [S-2-fluoro-alpha-methyl-4-biphenylacetic acid], a nonsteroidal anti-inflammatory drug, have been examined using steady-state and time-resolved spectroscopic techniques. The energy of its first singlet excited state is 99 kcal mol(-1). The fluorescence quantum yields and lifetimes (at 300 nm) have been determined in acetonitrile, methanol, hexane and PBS; they are in the range 0.15相似文献   

Spectroscopic investigations of the single tryptophan residue and of riboflavin and 7-oxolumazine bound to lumazine apoprotein from Photobacterium leiognathi

Spectroscopic techniques have been applied to investigate the conformation, local structure, and dynamic properties of the apoprotein of the lumazine protein from Photobacterium leiognathi and the holoprotein reconstituted with either the natural ligand 6,7-dimethyl-8-ribityllumazine or the closely related analogues riboflavin and 6-methyl-7-oxo-8-ribityllumazine (7-oxolumazine). The analogues are bound similarly to the natural prosthetic group. They exhibit similar shifts on binding in their absorption and fluorescence spectra, single-exponential fluorescence decays, and no independent motion from the protein as evident from a long-lived anisotropy decay (single-exponential phi = 10 ns, 20 degrees C) and high initial anisotropy. Steady-state anisotropy measurements result in similar KD's (40 nM, 20 degrees C, 50 mM inorganic phosphate) for all ligands. Circular dichroism in the far-UV region (190-250 nm) indicates no change in secondary structure on binding to the apoprotein. In the spectral region of 250-310 nm relatively large changes occur, indicating changes in the environment of the tyrosine and tryptophan residues. The single tryptophan residue shows a three-exponential decay of its fluorescence in both the apoprotein and the holoprotein. Radiationless energy transfer also occurs from the tryptophan to the bound ligand, especially evident with 7-oxolumazine. We have designed a new method for evaluation of the rate constant of energy transfer by measuring the (picosecond) rise time of the acceptor fluorescence. The anisotropy decay of the tryptophan residue shows two correlation times, a short one (phi approximately equal to 0.4 ns) representing rapid but restriced oscillation of this residue and a longer one (phi 2 = 5-7 ns, 20 degrees C) representing the motion of a larger segment of the protein.     

Bioluminescence spectral and fluorescence dynamics study of the interaction of lumazine protein with the intermediates of bacterial luciferase bioluminescence

The mechanism of the shifting of the bioluminescence spectrum from the reaction of bacterial luciferase by lumazine protein is investigated by methods of fluorescence dynamics. A metastable intermediate is produced on reaction of Vibrio harveyi luciferase with FMNH2 and O2. It has an absorption maximum at 374 nm and a rotational correlation time (phi) derived from the decay of its fluorescence (maximum 500 nm) anisotropy of 90 ns (2 degrees C). Lumazine protein from Photobacterium phosphoreum has an absorption maximum at 417 nm and a fluorescence maximum at 475 nm. Lumazine protein forms a protein-protein complex with luciferase, and the complex has a phi of approximately 100 ns. A mixture of lumazine protein and the intermediate would be expected to have an average correlation time (phi av) around 100 ns, but instead, the result is anomalous. The phi av is much lower and is also wavelength dependent. For excitation at 375 nm, which is mainly absorbed in the flavin chromophore of the intermediate, phi av = 25 ns, but at 415 nm, mainly absorbed by the lumazine derivative ligand of lumazine protein, phi av approximately 50 ns. It is proposed that protein-protein complexation occurs between lumazine protein and the luciferase intermediate and that in this complex energy transfer from the flavin to the lumazine is the predominant channel of anisotropy loss. A distance of 20 A between the donor and acceptor is calculated. In the bioluminescence reaction of intermediate with tetradecanal, a fluorescent transient species is produced which is the bioluminescence emitter.(ABSTRACT TRUNCATED AT 250 WORDS)     

Nanosecond fluorescence anisotropy decays of 1,6-diphenyl-1,3,5-hexatriene in membranes.

Nanosecond decays of the fluorescence anisotropy, r, were studied for the emission of 1,6-diphenyl-1,3,5-hexatriene (DPH) embedded in a series of mixed multilamellar liposomes containing egg yolk phosphatidylcholine, phosphatidylethanolamine and cholesterol in varying molar ratios, as well as in membranes of intact cells and in virus envelopes. The relative contributions of the fast and the infinitely slow decaying component to the steady-state value r, of the fluorescence anisotropy were very similar for artifical and biological membranes. Angles, theta, of the cone, by which the motion of the fluorescent molecule is limited, were calculated from the intensity of the infinitely slow decaying anisotropy component and compared with steady-state fluorescence anisotropies and with 'microviscosities', (eta). An increase in (eta) from 1.5 to 5.2 P in our systems was accompanied by a decrease in theta from 49 degrees to 30 degrees while the decrease in the mean motional relaxation times, phi f, of the label molecule was not more than 1 ns and due mainly to changes in the potential, by which the diffusion of DPH in the membrane is restricted. From these observations we conclude that differences in the steady-state fluorescence anisotropy and in 'microviscosities' of cholesterol-containing membranes (r greater than 0.15) represent changes in the degree of static orientational constraint rather than changes in diffusion rates of the label.     

Tryptophan fluorescence of terminal deoxynucleotidyl transferase: effects of quenchers on time-resolved emission spectra

Terminal deoxynucleotidyl transferase (EC 2.7.7.31) is a eucaryotic DNA polymerase that does not require a template. The tryptophan environments in calf thymus terminal transferase were investigated by fluorescence. The heterogeneous emission from this multitryptophan enzyme was separated by time-resolved emission spectroscopy. Nanosecond fluorescence decays at 296-nm excitation and various emission wavelengths were deconvolved by global analysis, assuming that the lifetimes but not the relative weighting factors were independent of emission wavelength. The data were fit to three exponentials of lifetimes tau 1 = 1.4 ns, tau 2 = 4.5 ns, and tau 3 = 7.7 ns. The corresponding decay-associated emission spectra of the three components had maxima at about 328, 335, and 345 nm. The accessibility of individual tryptophan environments to polar and nonpolar fluorescence quenchers was examined in steady-state and time-resolved experiments. In the presence of iodide and acrylamide, the steady-state emission spectra shift to the blue. However, at low quencher concentrations, the emission from the 7.7-ns component (maximum 345 nm) is hardly affected, suggesting that this hydrophilic tryptophan environment is buried within the protein. On the other hand, the red shift in the steady-state emission spectrum in the presence of trichloroethanol indicates that the 1.4-ns component (maximum 328 nm) is an exposed hydrophobic tryptophan environment. The results are consistent with an inside-out model for terminal transferase protein, with the more hydrophobic tryptophan(s) near the surface and the most hydrophilic tryptophan(s) in the core.     

Kinetic studies on the helix-coil transition of fluorescent labeled poly(-L-lysine) by the temperature-jump technique

Fluorescent dansyl labels were covalently attached to poly (L-lysine) (poly(Lys)) with a degree of polymerization of 300 to 600. The degree of labeling was 0.01 to 0.085 (mol label to mol amino acid residues). From the decay of the anisotropy of fluorescence it was concluded that the labels were highly mobile both in the coiled and helical state. A decrease of fluorescence intensity accompanied the helix-coil transition. Identical pH induced transition curves were measured by circular dichroism and fluorescence. The midpoint of the transition was at pH 10.2. The kinetics of the transition were studied by temperature-jump relaxation using fluorescence detection. A single relaxation phase was observed. The relaxation time tau exhibited a distorted bell shaped dependence on the degree of helicity f with a maximum value tau(max) = 15 micros at f = 0.3 and 20 degrees C. It was independent of polymer concentration and of the degree of labeling. A rate constant of helix propagation kF = 10(7) s(-1) was calculated from tau(max) and published values of the nucleation parameter sigma. The activation energy was 16 kJ mol . The observed rate constant is comparable to that of poly(L-glutamic acid) but two orders of magnitude smaller than that found for polyamino acids with nonionizable side chains.